Abstract
In this paper, the effects of channel roughness on the droplet removal efficiency and pressure drop in a zigzag mist eliminator are investigated. The fluid flow, droplet dispersion and deposition through the demister are modelled using a commercial Computational Fluid Dynamics (CFD) tool. The turbulent airflow is simulated using two different Shear-stress Transport (SST) k-ω model and Reynolds Stress Model (RSM) with enhanced wall treatment. The Eddy Interaction Model (EIM) is also used to predict the trajectories of the droplets in the gas flow. The results show that inserting roughness increases the maximum velocity of the gas flow at the bends and enhances the removal efficiency with a little cost of an increase in the pressure drop for each bend. At the velocity inlet of 2 m/s with 6 μm droplets, the pressure drop and removal efficiency of the threaded zigzag demister with 5 threads increases by 22.7% and 16.08 %, respectively. Moreover, a higher value for the figure of merit is achieved for the threaded demister compared with the smooth unit which means that the effect of higher removal efficiency of the threaded unit is more pronounced than the effect of higher pressure drop showing the advantages of adding threads in demisters.
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Abbreviations
- \( C_{D} \) :
-
Drag coefficient [-]
- \( C_{L} \) :
-
Discrete phase model constant [-]
- \( d \) :
-
Droplet diameter [μm]
- \( D_{\omega } \) :
-
Cross-diffusion term [kg/m3s2]
- \( F_{D} \) :
-
Coefficient in drag force calculation [1/s]
- \( F_{x} \) :
-
Additional acceleration [m/s2]
- \( g_{x} \) :
-
Gravitational acceleration [m/s2]
- \( \tilde{G}_{k} \) :
-
Production of turbulence kinetic energy [kg/ms3]
- \( G_{k} \) :
-
Production of turbulence kinetic energy [kg/ms3]
- \( G_{\omega } \) :
-
Production of ω [kg/m3s2]
- \( k \) :
-
Turbulence kinetic energy [m2/s2]
- \( L_{e} \) :
-
Eddy length scale [m]
- \( n \) :
-
Number of bends [-]
- \( r \) :
-
Random number [-]
- \( \text{Re}_{r} \) :
-
Relative Reynolds number [-]
- \( \text{Re}_{ij} \) :
-
Reynolds stress tensor [m2/s2]
- \( s \) :
-
Surface of sphere with same volume [m2]
- \( S \) :
-
Actual surface of the droplet [m2]
- \( S \) :
-
Width of the demister channel [mm]
- \( S_{\varphi } \) :
-
Source term in transport equation
- \( t_{cross} \) :
-
Droplet eddy crossing time [s]
- \( T_{L} \) :
-
Integral time [s]
- \( u^{\prime} \) :
-
Fluctuation of gas flow velocity [m/s]
- \( \bar{u} \) :
-
Mean fluid phase velocity [m/s]
- \( u \) :
-
Fluid phase velocity [m/s]
- \( u_{p} \) :
-
Droplet velocity [m/s]
- \( Y_{k} \) :
-
Dissipation of kinetic energy [kg/ms3]
- \( Y_{\omega } \) :
-
Dissipation of ω [kg/m3s2]
- \( \varGamma_{k} \) :
-
Effective diffusivity of kinetic energy [kg/ms]
- \( \varGamma_{\omega } \) :
-
Effective diffusivity of \( \omega \) [kg/ms]
- \( \varGamma_{\varphi } \) :
-
Diffusion coefficient in transport equation
- \( \eta \) :
-
Droplet removal efficiency [%]
- \( \eta_{B} \) :
-
Efficiency of each bend [%]
- \( \alpha \) :
-
Bend angle [-]
- \( \varepsilon \) :
-
Dissipation rate [m2/s3]
- \( \lambda \) :
-
Bend wavelength [mm]
- \( \mu_{t} \) :
-
Turbulent viscosity [kg/ms]
- \( \mu \) :
-
Molecular viscosity of the fluid [kg/ms]
- \( \rho_{p} \) :
-
Droplet density [kg/m3]
- \( \rho \) :
-
Gas density [kg/m3]
- \( \rho_{d} \) :
-
Droplet density [kg/m3]
- \( \sigma_{k} \) :
-
Turbulent Prandtl number for k [-]
- \( \sigma_{\omega } \) :
-
Turbulent Prandtl number for ω [-]
- \( \tau \) :
-
Droplet relaxation time [s]
- \( \nu \) :
-
Gas bulk velocity at inlet [m/s]
- \( \omega \) :
-
Specific dissipation rate [1/s]
- \( \phi \) :
-
Shape factor [-]
- \( \varsigma \) :
-
Normally distributed random number [-]
- \( \varphi \) :
-
General variable in transport equation
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Alamshahi, F., Rahimzadeh, H., Rafee, R. et al. Effects of Roughness on the Performance of a threaded Zigzag Demister Using RSM and k − ω turbulent models. Sādhanā 45, 283 (2020). https://doi.org/10.1007/s12046-020-01510-2
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DOI: https://doi.org/10.1007/s12046-020-01510-2